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Slack tide
Slack tide
from Wikipedia

Slack tide or slack water is the short period in a body of tidal water when the water is completely unstressed, and there is no movement either way in the tidal stream. It occurs before the direction of the tidal stream reverses.[1] Slack water can be estimated using a tidal atlas or the tidal diamond information on a nautical chart.[2] The time of slack water, particularly in constricted waters, does not occur at high and low water,[3] and in certain areas, such as Primera Angostura, the ebb may run for up to three hours after the water level has started to rise. Similarly, the flood may run for up to three hours after the water has started to fall. In 1884, Thornton Lecky illustrated the phenomenon with an inland basin of infinite size, connected to the sea by a narrow mouth. Since the level of the basin is always at mean sea level, the flood in the mouth starts at half tide, and its velocity is at its greatest at the time of high water, with the strongest ebb occurring conversely at low water.[4]

Implications for seafarers

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For scuba divers, the absence of a flow means that less effort is required to swim and there is less likelihood of drifting away from a vessel or shore. Slack water following high tide can improve underwater visibility, as the previously incoming tide brings clear water with it. Following low tide, visibility can be reduced as the ebb draws silt, mud, and other particulates with it. In areas with potentially dangerous tides and currents, it is standard practice for divers to plan a dive at slack times.

For any vessel, a favourable flow will improve the vessel's speed over the bottom for a given speed in the water. Difficult channels are also more safely navigated during slack water, as any flow may set a vessel out of a channel into danger.

Combined tidal stream and current

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In many locations, in addition to the tidal streams there is also a current causing the tidal stream in the one direction to be stronger than, and last for longer than the stream in the opposite direction six hours later. Variations in the strength of that current will also vary the time when the stream reverses, thus altering the time and duration of slack water. Variations in wind stress also directly affect the height of the tide, and the inverse relationship between the height of the tide and atmospheric pressure is well understood (1 cm change in sea level for each 1 mb change in pressure) while the duration of slack water at a given location is inversely related to the height of the tide at that location.

Misconceptions

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Slack water is different from the 'stand of the tide', which is when tide levels 'stand' at a maximum or minimum (i.e., at that moment in time, not rising or falling).[5]

Dodge tides

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Some localities have unusual tidal characteristics, such as Gulf St Vincent, South Australia, where the amplitudes of the main semi-diurnal tide constituents are almost identical. At neap tides the semi-diurnal tide is virtually absent, resulting in the phenomenon known as a "dodge tide"[6][7]—a day-long period of slack water—occurring twice a month; this effect is accentuated near the equinoxes when the diurnal component also vanishes, resulting in a period of 2–3 days of slack water.[8][9][10]

See also

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  • Stability theory, a main mathematical concept considering forces in equilibrium.

References

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Revisions and contributorsEdit on WikipediaRead on Wikipedia
from Grokipedia
Slack tide, also known as slack , is the short period during a tidal cycle when the tidal current's is at its minimum, typically approaching or reaching zero, as the transitions between the incoming current and the outgoing ebb current. This phenomenon occurs twice in each approximately 12-hour-and-25-minute tidal cycle, separating the phases of movement driven by gravitational forces from the and Sun. The duration of slack tide varies by location, often lasting from a few minutes to about an hour, and is influenced by factors such as , the phase of the , wind conditions, and the type of tidal regime—such as standing waves, where slack aligns closely with high or low water, or progressive waves, where it occurs midway between them. It is distinct from the stand of the tide, which refers to the interval around high or low water when there is minimal change in , though the two may coincide in some areas but not others due to local hydrodynamic effects. Slack tide holds practical significance for and , offering a brief window of relatively still water that reduces risks associated with strong currents in estuaries, inlets, and , where tidal flows can otherwise exceed several kilometers per hour. Boaters often prefer this period for docking or maneuvering, as the absence of significant current simplifies handling, provided wind influences are accounted for. In activities like , , and certain types of , slack tide minimizes water movement, enhancing safety and efficiency.

Definition and Characteristics

Definition of Slack Tide

Slack tide, also known as slack water, is the short period in a tidal cycle when the tidal current velocity is at its minimum, typically approaching or reaching zero, as the water transitions between the incoming current and the outgoing ebb current. This phenomenon represents the transition between the rising and falling ebb phases of the , where the horizontal movement of water effectively halts, creating a state of relative calm in current flow. The duration of slack tide varies by location, often lasting from a few minutes to about an hour, influenced by factors such as and local geography. During slack tide, the tidal current is in an unstressed condition, characterized by negligible horizontal flow due to the tidal component, although some residual non-tidal currents may persist depending on site-specific dynamics. This physical state underscores the temporary balance of forces driving tidal currents, distinguishing it as a key phase in tidal cycles. The term "slack tide" originates from 18th-century nautical , where "slack" denoted looseness or lack of tension, applied to the calm period without active tidal flow, as opposed to the stronger incoming or outgoing currents. Slack tide is precisely defined and measured by the near-zero velocity of the tidal current, observed using current meters, acoustic Doppler current profilers, or visual assessments of water flow, often appearing as minimal movement in tidal current records. Such measurements provide essential data for verifying the onset and end of slack tide, ensuring accurate delineation in tidal analyses.

Occurrence in the Tidal Cycle

In regions with semi-diurnal , slack tide occurs twice each , once near the time of high water at the end of the current and once near low water at the end of the ebb current. This pattern aligns with the two high and two low characteristic of semi-diurnal cycles, where the reversal of flow marks the brief interval of minimal current . The timing of slack tide relative to high and low varies by location and tidal regime: in systems, it occurs near high or low , while in progressive wave systems, it happens midway between them. The duration of slack tide varies depending on tidal strength, typically lasting from a few minutes to about an hour. During spring tides, when gravitational forces from the sun and are aligned, stronger currents accelerate the transition between flood and ebb, resulting in shorter slack periods. In contrast, neap tides, occurring when the sun and are at right angles, produce weaker overall tidal movements and extended slack water durations, sometimes approaching an hour or more as the semi-diurnal component diminishes. Slack tides are synchronized with the moon's position relative to Earth, completing a full cycle every of approximately 24 hours and 50 minutes, causing successive high and low waters—and thus slacks—to occur about 50 minutes later each calendar day. Globally, slack tides are most predictable and frequent in coastal areas dominated by semi-diurnal regimes, such as the Atlantic coasts of and . In diurnal tide regions, like parts of the or , slack water may occur only once per or irregularly due to the single high and low tide pattern, often with prolonged weak currents.

Underlying Mechanisms

Tidal Forces and Dynamics

The gravitational forces driving tides primarily arise from the Moon and the Sun, with the Moon exerting the dominant influence due to its proximity to Earth. The Moon's tidal force is approximately 2.2 times that of the Sun, contributing about 69% to the total tidal effect, while the Sun accounts for roughly 31%. These forces create two tidal bulges on Earth: one facing the Moon (or Sun) due to direct gravitational attraction and another on the opposite side resulting from the centrifugal force of the Earth-Moon (or Earth-Sun) orbital motion. As Earth rotates, an observer experiences alternating high and low water levels, with high and low water occurring at the moments of maximum and minimum elevation when the rate of change in water level is zero. Slack tide, the period of minimal tidal current, emerges in dynamic models as the transition between flood and ebb, though in the simplified equilibrium theory, horizontal currents are not explicitly modeled. In the equilibrium tide theory, a simplified model assumes that the ocean surface instantly adjusts to the tidal potential generated by these gravitational and centrifugal forces, forming a static ellipsoidal shape aligned with the perturbers. This theory, originally developed by Newton and refined by Laplace, neglects ocean inertia and friction but provides a foundational understanding of tidal periodicity. The tidal potential VV at a point on Earth's surface can be approximated by the second-order term in the multipole expansion: VGMd(rd)23cos2ψ12,V \approx -\frac{GM}{d} \left( \frac{r}{d} \right)^2 \frac{3 \cos^2 \psi - 1}{2}, where GG is the gravitational constant, MM and dd are the mass and distance of the Moon (or Sun), rr is the distance from Earth's center, and ψ\psi is the angular separation between the point and the perturber's direction. Equilibrium at high and low water points occurs where the vertical gradient V/z=0\partial V / \partial z = 0, corresponding to the extrema of the potential. Real oceanic tides deviate from the equilibrium model due to dynamic effects, including frictional dissipation, the from , and within ocean basins. Friction dampens wave propagation and distorts tidal amplitudes, while the Coriolis effect deflects tidal flows, leading to rotary motion rather than linear oscillation. Basin amplifies tides when the tidal period matches the natural oscillation frequency of semi-enclosed seas, such as the . These factors modify the timing and duration of slack tides, often shortening or elongating them compared to ideal predictions. Amphidromic systems further illustrate these dynamics, featuring a central node (amphidromic point) of zero around which the tidal crest rotates like a wave propagating from the node. This rotation arises from the balancing inertial and frictional forces in bounded basins, causing co-tidal lines (lines of constant high-water phase) to radiate outward and co-range lines (amplitude contours) to form concentric circles. As a result, slack tides occur at progressively later times with distance from the node, explaining regional variations; for example, in the , the M2 tidal amphidrome near results in a counterclockwise progression of slacks around the .

Distinction from Slack Water

Slack water is a for slack tide, referring to the period during the tidal cycle when the velocity of the tidal stream—the horizontal component of water movement—is minimal or near zero, marking the transition between and ebb currents. While terminology can vary in some nautical contexts, where "slack tide" may occasionally refer to the stabilization of at high or low tide, standard oceanographic usage aligns them as the same phenomenon focused on the cessation of horizontal flow. In many coastal areas, slack water (or slack tide) does not coincide exactly with high or low tide due to local factors such as channel morphology, bottom friction, and the propagation of tidal waves. Typically, slack precedes or follows high or by 10 to 30 minutes; for example, in , it can occur up to 30 minutes after the peak water level. These offsets arise because the horizontal current responds to the created by the tilting water surface, which lags slightly behind the vertical level change in confined or irregular waterways. The interplay between these components is analyzed through vector representations of tidal currents, where the tidal stream constitutes the horizontal vector of overall water motion, and the represents the vertical oscillation driven by gravitational forces. The full tidal current integrates both, but slack water specifically isolates the point of minimal horizontal velocity, often requiring for precise modeling in or hydrodynamic studies. Predictions for slack tide are derived from tidal current tables, which forecast horizontal flow speeds and directions based on . In contrast, tide tables predict vertical water levels. Local variations require measurements from current meters. Regional differences amplify these distinctions; in narrow straits like those in the , offsets between slack water and high or low can exceed one hour due to amplified frictional effects and constricted flow paths, significantly impacting tidal predictions for safe passage.

Types and Variations

High and Low Water Slacks

High water slack occurs at the peak of the tidal cycle, when the water level reaches its maximum height and tidal currents approach zero, resulting in a relatively calm surface. Low water slack, in contrast, takes place at the minimum tidal level, where currents similarly diminish to near zero, often leading to greater exposure of the in intertidal zones. The durations of these slacks differ notably and depend on tidal asymmetry; high water slacks tend to be longer in flood-dominant regimes, while low water slacks may persist longer in ebb-dominant systems or shallow basins, sometimes extending up to an hour or more depending on local morphology. Predicting the precise timing of these zero-velocity points relies on , which decomposes tidal signals into sinusoidal constituents to forecast both water levels and currents. The tidal height is modeled as h(t)=H0+i=1NHicos(ωit+ϕi),h(t) = H_0 + \sum_{i=1}^{N} H_i \cos(\omega_i t + \phi_i), where H0H_0 is the mean level, HiH_i the amplitude, ωi\omega_i the angular frequency, and ϕi\phi_i the phase of each constituent ii. Slack times are then identified by solving for when the corresponding velocity function u(t)=0u(t) = 0, incorporating similar harmonic terms for current speed. High water slacks often facilitate marine activities such as diving or anchoring due to minimal current interference, while low water slacks can enhance sediment exposure, briefly altering benthic habitats. These durations and behaviors vary with neap and spring cycles, where spring tides generally produce shorter slacks overall.

Dodge Tides

Dodge tides refer to extended periods of slack water lasting up to 24-48 hours, characterized by minimal and negligible water level fluctuations, typically occurring during neap tides when the gravitational forces of the sun and partially counteract each other. These conditions result in high and low tides being nearly indistinguishable, with water levels remaining almost constant over one or two days, distinguishing them from standard short-duration slacks. The term "dodge tide" was coined by British navigator in 1802 during his surveys of 's coastline, particularly in the shallow waters of , where he observed that seemed to evade their expected rise and fall. The name "dodge" evokes the idea of the tide avoiding or dodging movement, reflecting Flinders' frustration with these unpredictable calms during . This terminology remains unique to , though similar prolonged weak neap conditions occur elsewhere under different names. Dodge tides arise primarily from the near-equal amplitudes of the principal lunar semi-diurnal (M₂) and solar semi-diurnal (S₂) tidal constituents in the region, which align in opposition during neap cycles, effectively canceling the semi-diurnal signal and reducing overall tidal amplitude. In , M₂ amplitudes range from 38-50 cm and S₂ from 39-49 cm, leading to a neap semi-diurnal range approximated by the difference in these components, often exacerbated by local variations and winds. This alignment produces an approximate neap amplitude reduction modeled as 0.58 times the lunar component plus 0.41 times the solar component, reflecting the relative strengths in the tidal forcing. These phenomena are most prevalent in the enclosed, shallow basin of , where resonance and frictional effects amplify the near-cancellation, occurring roughly twice monthly in sync with neap phases but less frequently than typical flat neaps due to the specific harmonic balance. tides can be predicted using in tide tables, identified as days with tidal ranges below 0.5 m, aided by modern numerical models from agencies like the . While analogous weak neaps appear in other mixed- regimes globally, the extended duration and local naming make dodge tides a distinctive feature of this Australian gulf.

Implications and Applications

Maritime Navigation

Slack tide provides significant advantages for maritime navigation by minimizing tidal currents, which typically range from 0 to 1 during this period compared to peak flows of up to 4-5 knots in areas like . This reduced current facilitates easier maneuvering in narrow channels and confined waters, allowing vessels to maintain precise control without excessive rudder adjustments or engine power. Additionally, the calm conditions during slack tide can lower consumption by reducing the need for compensatory thrust against opposing streams in tidal . Safer anchoring is also enabled, as the absence of current drift minimizes veering and improves holding reliability, particularly in exposed anchorages. Mariners employ timing strategies to align vessel movements with slack tide, planning transits through high-current areas to coincide with these windows, which often last 20-60 minutes depending on location and lunar phase. Nautical almanacs such as Reeds Nautical Almanac provide detailed predictions of slack times derived from harmonic analysis, enabling route optimization for both recreational and commercial craft. These strategies are essential in regions with rotary tidal flows, where failing to time slack can extend passage times by hours against adverse currents reaching 4 knots or more. Mistiming slack tide poses substantial risks, as the rapid onset of strong tidal streams—often accelerating to 3-5 knots within minutes—can overwhelm vessel control, leading to grounding on shoals or uncontrolled drift toward hazards. These events underscore the peril of post-slack acceleration, where even modern vessels risk collision or stranding if engine power or steerage is insufficient. Tools for slack tide prediction integrate traditional and digital methods to enhance accuracy and real-time awareness. GPS-equipped devices, often paired with tide apps like those from NOAA, calculate local slack times using positional data and harmonic constants, allowing dynamic adjustments during transit. VHF radio broadcasts, including on channels 22A and 16, disseminate tidal current forecasts from coastal stations, providing mariners with updates on slack intervals up to 20 nautical miles offshore. (IHO) standards, outlined in S-44 and related resolutions, govern the format and reliability of electronic tidal current predictions in navigational charts, ensuring global consistency for slack water data. In commercial operations, slack tide optimization directly impacts efficiency across sectors. Ferry schedules in tidal-dependent routes, such as those in the , are calibrated to slack periods to minimize delays and fuel costs, with trajectory models showing up to 3.5% time savings in strong stream avoidance. Fishing fleets leverage slack predictions to position nets or trawls with reduced drift, improving catch rates by 15-25% in current-sensitive grounds through integrated tidal data. Ongoing advancements in models from NOAA continue to improve predictions for slack tide in variable tidal environments.

Environmental and Ecological Effects

During slack tide, tidal currents reach a minimum, temporarily halting erosion and deposition processes in coastal and estuarine environments. This pause allows fine suspended particles to settle, forming temporary drapes or stabilizing bedforms, which reduces overall resuspension compared to active or ebb phases. As a result, turbidity decreases, improving clarity and enabling greater light penetration for benthic in beds and algal communities. Slack tide provides critical foraging opportunities for intertidal species, as reduced water flow exposes habitats and minimizes disturbance. For instance, shorebirds and crabs, such as fiddler crabs (Uca pugilator), exploit these low-turbulence periods to feed on exposed infauna and detritus along mudflats. Additionally, the diminished currents facilitate larval settlement in estuaries by allowing planktonic stages of crustaceans and bivalves to descend and attach to substrates without being swept away, enhancing recruitment success for species like shore crabs (Carcinus maenas). In terms of water quality, slack tide limits vertical and horizontal mixing, thereby reducing the dispersion of pollutants from point sources such as or industrial discharges into broader marine areas. This containment can prevent widespread , while oxygen levels in the stabilize due to decreased of hypoxic bottom waters, providing respite for and supporting higher dissolved oxygen thresholds essential for aquatic respiration. Sea-level rise, accelerating at rates up to 5 mm/year in recent decades, alters tidal dynamics by increasing the tidal prism and shifting asymmetries, which can shorten or prolong slack tide durations depending on local and inlet morphology. These changes exacerbate risks, as elevated mean levels make high-water slacks more prone to inundation, amplifying the of tidal overflows in low-lying areas by 300-900% compared to pre-1970 baselines. In mangrove ecosystems, slack tides play a key role in retention by slowing currents to near-zero velocities, promoting the and deposition of organic-rich sediments laden with nutrients like and . A from the Kemaman River in demonstrates this, where slack periods during monsoons enable monthly sediment accretion rates of 2.6 mm, trapping flocs that would otherwise be resuspended during ebb and supporting mangrove productivity through enhanced . Similarly, in subtropical estuaries, mangroves function as dynamic sinks for during slack-influenced tidal exchanges, reducing downstream loading by up to 20-30% and mitigating in adjacent waters.

Misconceptions and Clarifications

Common Misunderstandings

One common misunderstanding equates slack tide with a complete absence of water movement, implying zero current in all directions. In reality, slack tide refers specifically to the period when the tidal current reaches its minimum speed, typically near zero for the reversing tidal flow, but non-tidal horizontal flows—such as those driven by wind, river discharge, or density gradients—can persist and influence navigation or boating conditions. This distinction is important, as assuming total stillness can lead to underestimating residual currents in areas like estuaries or coastal zones. Another prevalent error assumes slack tide occurs at uniform times globally, often based on simplified tide charts that overlook regional tidal regimes. Slack periods vary significantly due to diurnal (one high/low tide per day) versus semidiurnal (two equal high/low tides per day) patterns; for instance, the predominantly features mixed or diurnal tides with fewer slack events per cycle, while the Atlantic typically experiences semidiurnal tides with two slacks daily, shifting timings by hours across basins. These variations arise from amphidromic systems and basin geometry, making universal timing assumptions unreliable for planning activities like or . Slack tide is sometimes confused with periods of calm or flat seas, as if the phenomenon is meteorological rather than tidal. However, slack tide is a direct result of gravitational tidal forces causing current reversal, independent of or atmospheric conditions, although opposing can create surface calm that mimics slack or, conversely, stir up turbulence during it. This misconception can endanger mariners who attribute stillness solely to , ignoring underlying tidal dynamics. For terminological clarity, slack tide (or slack water) specifically denotes the tidal current lull, distinct from high/low water stands. Historical misconceptions about slack tide stem from 18th- and early 19th-century nautical charts and almanacs, which often relied on approximate "vulgar establishment" methods to predict , sometimes overstating slack durations for safety margins to avoid hazards in unfamiliar waters. These rough calculations, adding fixed intervals like 48 minutes post-new moon, led to over-reliance on predicted slacks and contributed to navigational errors in colonial-era voyages. In modern contexts, particularly as of , mobile apps and outdated prediction tools can exhibit inaccuracies for slack tide timing due to unaccounted climate-induced changes, such as sea-level rise altering tidal amplitudes and phases in coastal areas. For example, long-term observations show semidiurnal tides along North Atlantic coasts have amplified in some locations since the , shifting slack occurrences and rendering legacy models less precise. NOAA resources, including updated tide tables and educational FAQs, provide reliable corrections and emphasize verifying predictions against to mitigate these pitfalls. Spring tides, occurring when the sun, moon, and Earth align during full and new moons, result in amplified tidal ranges that produce stronger currents and consequently shorter, more abrupt slack periods compared to neap tides. This heightened energy accelerates the reversal of tidal flows, compressing the duration of calm water at high and low tide transitions, often to mere minutes in dynamic coastal systems. In contrast, neap tides, which arise during the moon's first and third quarters when solar and lunar gravitational forces partially cancel, generate smaller tidal ranges and weaker currents, leading to prolonged slack durations that can extend significantly and serve as precursors to more extreme slack events like dodge tides. Tidal bores and surges represent rare but intense disruptions to expected slack conditions, particularly in estuarine and riverine environments where incoming tides propagate upstream against the current. The in the , for instance, manifests as a surging wave front during high spring , abruptly initiating flood flows and eliminating the calm slack phase by rapidly elevating water levels over distances up to 30 kilometers. Such phenomena alter the typical calm by introducing turbulent, high-velocity water movement, preventing the stabilization of flows and posing hazards to during what would otherwise be a period of minimal current. Long-period tides, driven by orbital variations such as the 18.6-year lunar nodal cycle, introduce monthly and annual modulations to tidal amplitudes that influence the predictability of slack occurrences. This cycle causes gradual shifts in the inclination of the moon's orbit relative to Earth's , varying the strength of diurnal tidal components and thereby altering tidal ranges by up to about 30 centimeters in some regions, which in turn affects the timing and duration of slacks over multi-year scales. These long-term fluctuations complicate short-term forecasting models, as enhanced ranges during nodal peaks can shorten slacks similar to spring conditions, while minima extend them, impacting coastal planning and operations. Emerging research on indicates that global , projected to reach 0.3-1 meter by 2100, is compressing slack durations in many coastal and estuarine systems through altered hydrodynamic balances. Increased water depths reduce frictional damping on tidal waves, amplifying propagation speeds and shortening the time available for flow reversals in tide-dominated regions. This effect, compounded by the 18.6-year lunar cycle's interaction with rising baselines, exacerbates variability in high-tide flooding and challenges predictions of calm intervals.

References

  1. https://www.coastalwiki.org/wiki/Coastal_and_marine_sediments
  2. https://www.coastalwiki.org/wiki/Long-period_lunar_tides
  3. https://www.coastalwiki.org/wiki/Tidal_bore_dynamics
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